Three-Body $J^P = 0^+,1^+,2^+$ $B^* B^* \bar{K}$ Bound States
Manuel Pavon Valderrama

TL;DR
This paper predicts the existence of novel three-body bound states involving heavy mesons and baryons with a kaon or antikaon, based on universal features of short-range interactions and mass ratios, and explores conditions for Efimov states.
Contribution
It introduces specific predictions for three-body bound states in heavy hadron systems with large mass ratios and analyzes the potential for Efimov effect occurrence in these systems.
Findings
A $B^* B^* ar{K}$ bound state is predicted 30-40 MeV below threshold.
Two bound states are expected in the $ ext{Xi}_{bb} ext{Xi}_{bb} ar{K}$ system, at 50-90 MeV and 5-15 MeV below threshold.
Conditions for Efimov effect in heavy hadron-kaon systems are discussed.
Abstract
Three body systems with short-range interactions display universal features that have been extensively explored in atomic physics, but apply to hadron physics as well. Systems composed of two non-interacting identical particles (species H) of mass and a third particle (species P) of mass that interacts attractively with the other two have the property that they are more likely to bind for larger values of the mass ratio . This is particularly striking if the HHP system is in P-wave (while the interacting pair is in S-wave), in which case one would not normally expect the formation of a three body state. If we assume that the binds to form the heavy meson and notice that the mass ratio of the to is , concrete calculations indicate that there should be a three body bound state between …
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